Closest Approach & Wind-Airplane Problems — NEET Physics MCQs with Solutions
Free NEET Physics Closest Approach & Wind-Airplane Problems MCQs with step-by-step solutions (25 questions). Part of Relative Motion (1D and 2D). Practise online on Prepizo — no login needed.
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Questions with solutions
Q1 — Closest Approach & Wind-Airplane Problems · medium · theory
Two moving particles will COLLIDE if the position vector of one relative to the other is:
A. Constant in magnitude
B. Zero at the start
C. Perpendicular to the relative velocity
D. Always parallel (anti-parallel) to their relative velocity ✓ Correct
Solution: Collision condition: r⃗_rel stays along v⃗_rel (the relative velocity points from one particle straight at the other). Speed-trick: in the frame of one particle, the other must head directly at it.
Q2 — Closest Approach & Wind-Airplane Problems · easy · theory
In the reference frame of particle B, particle A (both moving uniformly) appears to move:
A. At rest always
B. In a circle
C. In a straight line with constant velocity v⃗_A − v⃗_B ✓ Correct
D. In a parabola
Solution: With both velocities constant, the relative velocity is constant, so the relative trajectory is a straight line.
Q3 — Closest Approach & Wind-Airplane Problems · medium · theory
The time of closest approach for two uniformly moving particles with initial separation r⃗₀ and relative velocity v⃗_rel is:
A. $t = -\dfrac{\vec{r}_0 \cdot \vec{v}_{rel}}{|\vec{v}_{rel}|^2}$ ✓ Correct
B. $t = \dfrac{\vec{r}_0 \times \vec{v}_{rel}}{|\vec{v}_{rel}|}$
C. $t = 0$
D. $t = \dfrac{|\vec{r}_0|}{|\vec{v}_{rel}|}$ always
Solution: Minimising |r⃗₀ + v⃗_rel t|² gives t = −(r⃗₀·v⃗_rel)/|v⃗_rel|². (t = r₀/v_rel only when they head straight at each other.)
Q4 — Closest Approach & Wind-Airplane Problems · medium · theory
The minimum (closest-approach) distance between two uniformly moving particles equals:
A. Zero always
B. The initial separation always
C. The component of separation along the relative velocity
D. The component of the initial separation perpendicular to the relative velocity ✓ Correct
Solution: In the relative frame the moving particle travels a straight line; the closest distance is the perpendicular from the other particle to that line: d_min = r₀ sinα.
Q5 — Closest Approach & Wind-Airplane Problems · easy · theory
An aeroplane's velocity relative to the ground equals:
A. Its airspeed minus ground speed
B. Its airspeed always
C. The wind velocity alone
D. Its velocity relative to the air PLUS the wind velocity ✓ Correct
Solution: v⃗_plane,ground = v⃗_plane,air + v⃗_air,ground — the wind adds vectorially to the plane's airspeed.
Q6 — Closest Approach & Wind-Airplane Problems · medium · theory
For a plane to fly due north when a wind blows from the west, the pilot must head:
A. Slightly west of north (into the wind) ✓ Correct
B. Due west
C. Slightly east of north
D. Due north
Solution: The heading must have a westward component to cancel the eastward push of the wind (from the west means blowing towards the east).
Q7 — Closest Approach & Wind-Airplane Problems · easy · theory
With a tailwind (wind along the direction of flight), the ground speed of a plane is:
A. Airspeed − wind speed
B. Unchanged
C. Airspeed + wind speed ✓ Correct
D. Zero
Solution: A tailwind adds directly: v_ground = v_air + v_wind; a headwind subtracts.
Q8 — Closest Approach & Wind-Airplane Problems · medium · theory
A stone dropped from a uniformly moving train, as seen by a passenger IN the train, falls:
A. In a circle
B. Backward horizontally
C. In a parabola
D. Straight down (vertical straight line) ✓ Correct
Solution: Relative to the train the stone has zero horizontal velocity, so it falls vertically. To a ground observer it is a parabola. Relative trajectory depends on the frame!
Q9 — Closest Approach & Wind-Airplane Problems · medium · theory
Two projectiles are in flight simultaneously (same g). The trajectory of one as seen from the other is a:
A. Circle
B. Straight line ✓ Correct
C. Parabola
D. Ellipse
Solution: Relative acceleration = g − g = 0, so the relative velocity is constant and the relative path is a straight line.
Q10 — Closest Approach & Wind-Airplane Problems · medium · theory
For two ships to avoid collision, an observer on one ship must see the other ship's bearing (direction):
A. Changing with time ✓ Correct
B. Always at 90°
C. Constant with decreasing range
D. Along the relative velocity
Solution: Constant bearing + closing range = collision course (r⃗_rel parallel to v⃗_rel). A changing bearing means they will pass clear — the mariner's rule.
Q11 — Closest Approach & Wind-Airplane Problems · easy · numerical
A plane's airspeed is 200 km/h due north with a 50 km/h tailwind from the south. Its ground speed is:
A. 200 km/h
B. 250 km/h ✓ Correct
C. 150 km/h
D. 206 km/h
Solution: Wind from the south blows northward (tailwind): v_ground = 200 + 50 = 250 km/h.
Q12 — Closest Approach & Wind-Airplane Problems · easy · numerical
A plane flies at airspeed 200 km/h due north while a 50 km/h wind blows towards the east. Its ground speed is:
A. ≈ 206 km/h ✓ Correct
B. 150 km/h
C. ≈ 194 km/h
D. 250 km/h
Solution: Perpendicular vectors: v = √(200² + 50²) = √42500 ≈ 206 km/h, tilted east of north.
Q13 — Closest Approach & Wind-Airplane Problems · medium · numerical
A plane with airspeed 100 m/s must fly due north against a 60 m/s wind blowing towards the east. The pilot must head west of north by an angle:
A. 45°
B. sin⁻¹(0.6) ≈ 37° ✓ Correct
C. cos⁻¹(0.6) ≈ 53°
D. tan⁻¹(0.6) ≈ 31°
Solution: The westward component must cancel the wind: 100 sinθ = 60 ⇒ sinθ = 0.6 ⇒ θ ≈ 37° west of north.
Q14 — Closest Approach & Wind-Airplane Problems · medium · numerical
For the previous plane (100 m/s airspeed, 60 m/s crosswind cancelled), the resultant ground speed due north is:
A. 60 m/s
B. 100 m/s
C. 40 m/s
D. 80 m/s ✓ Correct
Solution: v_north = √(100² − 60²) = √6400 = 80 m/s (6-8-10 triangle).
Q15 — Closest Approach & Wind-Airplane Problems · easy · numerical
Ship A is 10 km due east of ship B. A sails west at 6 km/h and B sails east at 4 km/h (towards each other). They will meet after:
A. 1.67 h
B. 5 h
C. 2.5 h
D. 1 h ✓ Correct
Solution: Closing speed = 6 + 4 = 10 km/h; t = 10/10 = 1 h. (Head-on: r⃗₀ ∥ v⃗_rel, so they collide.)
Q16 — Closest Approach & Wind-Airplane Problems · easy · numerical
Two particles are 100 m apart. One moves at 10 m/s directly towards the other, which moves at 6 m/s directly away. The first catches the second after:
A. 10 s
B. 6.25 s
C. 16.7 s
D. 25 s ✓ Correct
Solution: v_rel = 10 − 6 = 4 m/s (closing); t = 100/4 = 25 s.
Q17 — Closest Approach & Wind-Airplane Problems · medium · numerical
Ship A is 10 km north of ship B. A sails east at 3 m/s; B sails north at 4 m/s. The magnitude of B's velocity relative to A is:
A. 3.5 m/s
B. 1 m/s
C. 7 m/s
D. 5 m/s ✓ Correct
Solution: v⃗_BA = v⃗_B − v⃗_A = (0,4) − (3,0) = (−3, 4); |v_BA| = 5 m/s.
Q18 — Closest Approach & Wind-Airplane Problems · medium · numerical
Two straight roads cross at right angles. Car A approaches the crossing from the west at 30 m/s, currently 400 m away; car B approaches from the south at 40 m/s, currently 300 m away. Their separation is decreasing. The relative speed of A with respect to B is:
A. 70 m/s
B. 50 m/s ✓ Correct
C. 10 m/s
D. 35 m/s
Solution: v⃗_rel = (30, 0) − (0, 40) = (30, −40); |v_rel| = √(900 + 1600) = 50 m/s.
Q19 — Closest Approach & Wind-Airplane Problems · medium · numerical
For the same two cars (A: 400 m west of crossing at 30 m/s; B: 300 m south at 40 m/s), both reach the crossing at t = 400/30 ≈ 13.3 s and t = 300/40 = 7.5 s respectively. Do they collide at the crossing?
A. No — they reach the crossing at different times ✓ Correct
B. Yes — collision is guaranteed by the geometry
C. Cannot be determined
D. Yes — both reach together
Solution: A arrives at 13.3 s, B at 7.5 s — different times, so no collision at the crossing. Pitfall: intersecting PATHS do not mean collision; the times must match too.
Q20 — Closest Approach & Wind-Airplane Problems · medium · numerical
Particle B is initially 100 m due east of A. A moves east at 8 m/s; B moves east at 3 m/s. Their closest approach (and when) is:
A. 50 m at t = 10 s
B. 0 m at t = 12.5 s
C. 0 m, at t = 20 s (A catches B) ✓ Correct
D. 100 m always
Solution: v_rel = 8 − 3 = 5 m/s along the line joining them (r⃗₀ ∥ v⃗_rel) ⇒ they meet: t = 100/5 = 20 s, d_min = 0.
Q21 — Closest Approach & Wind-Airplane Problems · medium · numerical
Particle B is 20 m due north of particle A. A moves north at 5 m/s and B moves east at 5 m/s. The minimum separation between them is (√2 ≈ 1.41):
A. ≈ 14.1 m ✓ Correct
B. 10 m
C. 0 m
D. 20 m
Solution: v⃗_AB = (0,5) − (5,0) = (−5,5); the initial separation vector (0,20) makes 45° with v⃗_rel ⇒ d_min = 20 sin45° ≈ 14.1 m.
Q22 — Closest Approach & Wind-Airplane Problems · medium · numerical
In the previous problem (separation 20 m, |v_rel| = 5√2 m/s, 45° geometry), the time of closest approach is:
A. 2 s ✓ Correct
B. 2.83 s
C. 4 s
D. 1 s
Solution: t = (r₀ cosα)/|v_rel| = (20 × cos45°)/(5√2) = (20/√2)/(5√2) = 20/10 = 2 s. (Or t = −r⃗₀·v⃗_rel/|v_rel|² = 100/50 = 2 s.)
Q23 — Closest Approach & Wind-Airplane Problems · medium · numerical
A plane must reach a city 400 km due north in 1 h. A wind of 60 km/h blows towards the east. The required airspeed is (≈):
A. 340 km/h
B. ≈ 404 km/h ✓ Correct
C. 460 km/h
D. 400 km/h
Solution: Ground velocity must be 400 km/h north; heading must cancel 60 east: v_air = √(400² + 60²) ≈ 404 km/h.
Q24 — Closest Approach & Wind-Airplane Problems · easy · numerical
A bird flies at airspeed 10 m/s heading due east while a wind blows at 10 m/s towards the north. The bird's ground velocity is:
A. 20 m/s north-east
B. 10√2 ≈ 14.1 m/s towards the north-east ✓ Correct
C. 10√2 m/s towards the south-east
D. 10 m/s due east
Solution: Equal perpendicular components ⇒ resultant 10√2 m/s at 45° (north-east).
Q25 — Closest Approach & Wind-Airplane Problems · easy · numerical
With a 50 km/h headwind, a plane of airspeed 250 km/h covers 600 km (ground distance) in:
A. 3 h ✓ Correct
B. 2 h
C. 2.4 h
D. 4 h
Solution: Ground speed = 250 − 50 = 200 km/h; t = 600/200 = 3 h.